The Pauli Exclusion Principle — Question 2

Section 40-6 · Physics pages 6674–6675

Question 2 An antisymmetric two-electron state has a normalization fixed by orthogonality Let a and b be orthonormal one-electron spin orbitals. Consider Ψ(1, 2) = C[a(1)b(2) −b(1)a(2)], with C positive. The labels 1 and 2 include space and spin. a(1)b(2) b(1)a(2) − exchange Schematic; labels, not drawing lengths, specify the data. (a) Normalize the state. (b) Apply particle exchange and determine what happens if b is replaced by a.
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Question 2 - Solution An antisymmetric two-electron state has a normalization fixed by orthogonality a(1)b(2) b(1)a(2) − exchange (a) Method and calculation ∥Ψ∥2 = C2[⟨a|a⟩⟨b|b⟩+ ⟨b|b⟩⟨a|a⟩−2|⟨a|b⟩|2] = 2C2. C = 1/ √ 2 . (b) Interpretation and further calculation Ψ(2, 1) = −Ψ(1, 2) . b = a ⇒Ψ = C[a(1)a(2) −a(1)a(2)] = 0 ⇒duplicate occupation excluded . Physical check The zero function cannot be normalized. Exclusion concerns identical complete spin orbitals, so two electrons may share a spatial orbital if their spin states differ.

Question 2

An antisymmetric two-electron state has a normalization fixed by orthogonality

Let a and b be orthonormal one-electron spin orbitals. Consider Ψ(1,2)=C[a(1)b(2)−b(1)a(2)]\Psi(1,2)=C[a(1)b(2)-b(1)a(2)], with C positive. The labels 1 and 2 include space and spin.

Diagram shown in the original SVG worksheet.

  1. Normalize the state.

  2. Apply particle exchange and determine what happens if b is replaced by a.

Question 2 - Solution

An antisymmetric two-electron state has a normalization fixed by orthogonality

Diagram shown in the original SVG worksheet.

(a) Method and calculation

∥Ψ∥2=C2[⟨a|a⟩⟨b|b⟩+⟨b|b⟩⟨a|a⟩−2|⟨a|b⟩|2]=2C2.\|\Psi\|^2=C^2[\langle a|a\rangle\langle b|b\rangle+\langle b|b\rangle\langle a|a\rangle-2|\langle a|b\rangle|^2]=2C^2.C=1/2.\boxed{C=1/\sqrt2}.

(b) Interpretation and further calculation

Ψ(2,1)=−Ψ(1,2).\boxed{\Psi(2,1)=-\Psi(1,2)}.b=a⇒Ψ=C[a(1)a(2)−a(1)a(2)]=0⇒duplicate occupation excluded.b=a\Rightarrow\Psi=C[a(1)a(2)-a(1)a(2)]=0\Rightarrow\boxed{\text{duplicate occupation excluded}}.

Physical check

The zero function cannot be normalized. Exclusion concerns identical complete spin orbitals, so two electrons may share a spatial orbital if their spin states differ.